Astronomy and Astrophysics – Astronomy
Scientific paper
Oct 1996
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=1996apj...470..301m&link_type=abstract
Astrophysical Journal v.470, p.301
Astronomy and Astrophysics
Astronomy
9
Galaxies: Nuclei, Galaxies: Seyfert, Line: Profiles
Scientific paper
We present model line profiles of [O II] λ3727, [Ne III] λ3869, [O III] λ5007, [Fe VII] λ6087, [Fe X] λ6374, [O I] λ6300, Hα λ6563, and [S II] λ6731. The profiles presented here illustrate explicitly the pronounced effects that collisional de-excitation, and that spatial variations in both the ionization parameter and cloud column density, have on narrow-line region (NLR) model profiles. The above effects were included only qualitatively in a previous analytical treatment by Moore & Cohen. By making a direct correspondence between these model profiles and the analytical model profiles of Moore & Cohen, and by comparing with the observed profiles presented in a companion paper and also with those presented elsewhere in the literature, we strengthen some of the conclusions of Moore & Cohen. Most notably, we argue for constant ionization parameter, uniformly accelerated outflow of clouds that are individually stratified in ionization, and the interpretation of emission-line width correlations with ionization potential as a column density effect. For comparison with previous observational studies, such as our own in a companion paper, we also calculate profile parameters for some of the models, and we present and discuss the resulting line width correlations with critical density (n_cr_) and ionization potential (IP). Because the models we favor are those that produce extended profile wings as observed in high spectral resolution studies, the line width correlations of our favoured models are of particular interest. Line width correlations with n_cr_ and/or IP result only if the width parameter is more sensitive to extended profile wings than is the full width at half-maximum (FWHM). Correlations between FWHM and n_cr_ and/or IP result only after convolving the model profiles with a broad instrumental profile that simulates the lower spectral resolution used in early observational studies. The model in agreement with the greatest number of observational considerations has electron density decreasing outward from n_e_ ~ 10^6^ cm^-3^ to n_e_~10^2^ cm^-3^ and, due to collisional de-excitation effects in the lowest velocity clouds, it generates broad flat-topped profile peaks in the lines of lowest critical density (e.g., [O II] λ3727 and [S II] λλ6716,6731). Because the observed profile peaks of both low and high critical density lines are often very similar, our favored model requires a contribution to NLR emission-line spectra from low-velocity, low-density, and low-ionization gas not included in the model NLR.
Cohen Ross D.
Moore David
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